Polar Coordinate System
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Engineering Curves – I
Engineering Curves – I 1. Classification 2. Conic sections - explanation 3. Common Definition 4. Ellipse – ( six methods of construction) 5. Parabola – ( Three methods of construction) 6. Hyperbola – ( Three methods of construction ) 7. Methods of drawing Tangents & Normals ( four cases) Engineering Curves – II 1. Classification 2. Definitions 3. Involutes - (five cases) 4. Cycloid 5. Trochoids – (Superior and Inferior) 6. Epic cycloid and Hypo - cycloid 7. Spiral (Two cases) 8. Helix – on cylinder & on cone 9. Methods of drawing Tangents and Normals (Three cases) ENGINEERING CURVES Part- I {Conic Sections} ELLIPSE PARABOLA HYPERBOLA 1.Concentric Circle Method 1.Rectangle Method 1.Rectangular Hyperbola (coordinates given) 2.Rectangle Method 2 Method of Tangents ( Triangle Method) 2 Rectangular Hyperbola 3.Oblong Method (P-V diagram - Equation given) 3.Basic Locus Method 4.Arcs of Circle Method (Directrix – focus) 3.Basic Locus Method (Directrix – focus) 5.Rhombus Metho 6.Basic Locus Method Methods of Drawing (Directrix – focus) Tangents & Normals To These Curves. CONIC SECTIONS ELLIPSE, PARABOLA AND HYPERBOLA ARE CALLED CONIC SECTIONS BECAUSE THESE CURVES APPEAR ON THE SURFACE OF A CONE WHEN IT IS CUT BY SOME TYPICAL CUTTING PLANES. OBSERVE ILLUSTRATIONS GIVEN BELOW.. Ellipse Section Plane Section Plane Hyperbola Through Generators Parallel to Axis. Section Plane Parallel to end generator. COMMON DEFINATION OF ELLIPSE, PARABOLA & HYPERBOLA: These are the loci of points moving in a plane such that the ratio of it’s distances from a fixed point And a fixed line always remains constant. The Ratio is called ECCENTRICITY. (E) A) For Ellipse E<1 B) For Parabola E=1 C) For Hyperbola E>1 Refer Problem nos. -
Section 2.6 Cylindrical and Spherical Coordinates
Section 2.6 Cylindrical and Spherical Coordinates A) Review on the Polar Coordinates The polar coordinate system consists of the origin O,the rotating ray or half line from O with unit tick. A point P in the plane can be uniquely described by its distance to the origin r = dist (P, O) and the angle µ, 0 µ < 2¼ : · Y P(x,y) r θ O X We call (r, µ) the polar coordinate of P. Suppose that P has Cartesian (stan- dard rectangular) coordinate (x, y) .Then the relation between two coordinate systems is displayed through the following conversion formula: x = r cos µ Polar Coord. to Cartesian Coord.: y = r sin µ ½ r = x2 + y2 Cartesian Coord. to Polar Coord.: y tan µ = ( p x 0 µ < ¼ if y > 0, 2¼ µ < ¼ if y 0. · · · Note that function tan µ has period ¼, and the principal value for inverse tangent function is ¼ y ¼ < arctan < . ¡ 2 x 2 1 So the angle should be determined by y arctan , if x > 0 xy 8 arctan + ¼, if x < 0 µ = > ¼ x > > , if x = 0, y > 0 < 2 ¼ , if x = 0, y < 0 > ¡ 2 > > Example 6.1. Fin:>d (a) Cartesian Coord. of P whose Polar Coord. is ¼ 2, , and (b) Polar Coord. of Q whose Cartesian Coord. is ( 1, 1) . 3 ¡ ¡ ³ So´l. (a) ¼ x = 2 cos = 1, 3 ¼ y = 2 sin = p3. 3 (b) r = p1 + 1 = p2 1 ¼ ¼ 5¼ tan µ = ¡ = 1 = µ = or µ = + ¼ = . 1 ) 4 4 4 ¡ 5¼ Since ( 1, 1) is in the third quadrant, we choose µ = so ¡ ¡ 4 5¼ p2, is Polar Coord. -
Designing Patterns with Polar Equations Using Maple
Designing Patterns with Polar Equations using Maple Somasundaram Velummylum Claflin University Department of Mathematics and Computer Science 400 Magnolia St Orangeburg, South Carolina 29115 U.S.A [email protected] The Cartesian coordinates and polar coordinates can be used to identify a point in two dimensions. The polar coordinate system has a fixed point O called the origin or pole and a directed half –line called the polar axis with end point O. A point P on the plane can be described by the polar coordinates ( r, θ ), where r is the radial distance from the origin and θ is the angle made by OP with the polar axis. Several important types of graphs have equations that are simpler in polar form than in rectangular form. For example, the polar equation of a circle having radius a and centered at the origin is simply r = a. In other words , polar coordinate system is useful in describing two dimensional regions that may be difficult to describe using Cartesian coordinates. For example, graphing the circle x 2 + y 2 = a 2 in Cartesian coordinates requires two functions, one for the upper half and one for the lower half. In polar coordinate system, the same circle has the very simple representation r = a. Maple can be used to create patterns in two dimensions using polar coordinate system. When we try to analyze two dimensional patterns mathematically it will be helpful if we can draw a set of patterns in different colors using the help of technology. To investigate and compare some patterns we will go through some examples of cardioids and rose curves that are drawn using Maple. -
The Dual Theorem Relative to the Simson's Line
THE DUAL THEOREM RELATIVE TO THE SIMSON’S LINE Prof. Ion Pătrașcu Frații Buzești College, Craiova, Romania Translated by Prof. Florentin Smarandache University of New Mexico, Gallup, NM 87301, USA Abstract In this article we elementarily prove some theorems on the poles and polars theory, we present the transformation using duality and we apply this transformation to obtain the dual theorem relative to the Samson’s line. I. POLE AND POLAR IN RAPPORT TO A CIRCLE Definition 1. Considering the circle COR(,), the point P in its plane PO≠ and uuur uuuur the point P ' such that OP⋅= OP' R2 . It is said about the perpendicular p constructed in the point P ' on the line OP that it is the point’s P polar, and about the point P that it is the line’s p pole. Observations M 1. If the point P belongs to the circle, its polar is the tangent in P to the circle U COR(,). uuur uuuur P' Indeed, the relation OP⋅= OP' R2 gives that PP' = . OP 2. If P is interior to the circle, its polar p is a V line exterior to the circle. 3. If P and Q are two points such that p m(POQ )= 90o , and p,q are their polars, from the definition results that p ⊥ q . Fig. 1 Proposition 1. If the point P is external to the circle COR( , ) , its polar is determined by the contact points with the circle of the tangents constructed from P to the circle Proof Let U and V be the contact points of the tangents constructed from P to the circle COR( , ) (see fig.1). -
Polar Coordinates and Calculus.Wxp
Polar Coordinates and Calculus Recall that in the Polar coordinate system the coordinates ) represent <ß the directed distance from the pole to the point and the directed angle, counterclockwise from the polar axis to the segment from the pole to the point. A polar function would be of the form: ) . < œ 0 To find the slope of the tangent line of a polar graph we will parameterize the equation. ) ( Assume is a differentiable function of ) ) <œ0 0 ¾Bœ<cos))) œ0 cos and Cœ< sin ))) œ0 sin . .C .C .) Recall also that œ .B .B .) 1Þ Find the derivative of < œ # sin ) Remember that horizontal tangent lines occur when and that vertical tangent lines occur when page 1 2 Find the HTL and VTL for cos ) and sketch the graph. Þ < œ # " page 2 Recall our formula for the derivative of a function in polar coordinates. Since Bœ<cos))) œ0 cos and Cœ< sin ))) œ0 sin , we can conclude .C .C .) that œ.B œ .B .) Solutions obtained by setting < œ ! gives equations of tangent lines through the pole. 3Þ Find the equations of the tangent line(s) through the pole if <œ#sin #Þ) page 3 To find the arc length of a polar curve, you have two options. 1) You can use the parametrization of the polar curve: cos))) cos and sin ))) sin Bœ< œ0 Cœ< œ0 then use the arc length formula for parametric curves: " w # w # 'α ÈÐBÐ) ÑÑ ÐCÐ ) ÑÑ . ) or, 2) You can use an alternative formula for arc length in polar form: " <# Ð.< Ñ # . -
Art and Engineering Inspired by Swarm Robotics
RICE UNIVERSITY Art and Engineering Inspired by Swarm Robotics by Yu Zhou A Thesis Submitted in Partial Fulfillment of the Requirements for the Degree Doctor of Philosophy Approved, Thesis Committee: Ronald Goldman, Chair Professor of Computer Science Joe Warren Professor of Computer Science Marcia O'Malley Professor of Mechanical Engineering Houston, Texas April, 2017 ABSTRACT Art and Engineering Inspired by Swarm Robotics by Yu Zhou Swarm robotics has the potential to combine the power of the hive with the sen- sibility of the individual to solve non-traditional problems in mechanical, industrial, and architectural engineering and to develop exquisite art beyond the ken of most contemporary painters, sculptors, and architects. The goal of this thesis is to apply swarm robotics to the sublime and the quotidian to achieve this synergy between art and engineering. The potential applications of collective behaviors, manipulation, and self-assembly are quite extensive. We will concentrate our research on three topics: fractals, stabil- ity analysis, and building an enhanced multi-robot simulator. Self-assembly of swarm robots into fractal shapes can be used both for artistic purposes (fractal sculptures) and in engineering applications (fractal antennas). Stability analysis studies whether distributed swarm algorithms are stable and robust either to sensing or to numerical errors, and tries to provide solutions to avoid unstable robot configurations. Our enhanced multi-robot simulator supports this research by providing real-time simula- tions with customized parameters, and can become as well a platform for educating a new generation of artists and engineers. The goal of this thesis is to use techniques inspired by swarm robotics to develop a computational framework accessible to and suitable for both artists and engineers. -
9.-PARABOLA-THEORY.Pdf
10. PARABOLA 1. INTRODUCTION TO CONIC SECTIONS 1.1 Geometrical Interpretation Conic section, or conic is the locus of a point which moves in a plane such that its distance from a fixed point is in a constant ratio to its perpendicular distance from a fixed straight line. (a) The fixed point is called the Focus. (b) The fixed straight line is called the Directrix. (c) The constant ratio is called the Eccentricity denoted by e. (d) The line passing through the focus and perpendicular to the directrix is called the Axis. (e) The point of intersection of a conic with its axis is called the Vertex. Sections on right circular cone by different planes (a) Section of a right circular cone by a plane passing through its vertex is a pair of straight lines passing through the vertex as shown in the figure. (b) Section of a right circular cone by a plane parallel to its base is a circle. (c) Section of a right circular cone by a plane parallel to a generator of the cone is a parabola. (d) Section of a right circular cone by a plane neither parallel to a side of the cone nor perpendicular to the axis of the cone is an ellipse. (e) Section of a right circular cone by a plane parallel to the axis of the cone is an ellipse or a hyperbola. 3D View: Circle Ellipse Parabola Hyperbola Figure 10.1 1.2 Conic Section as a Locus of a Point If a point moves in a plane such that its distances from a fixed point and from a fixed line always bear a constant ratio 'e' then the locus of the point is a conic section of the eccentricity e (focus-directrix property). -
Classical Mechanics Lecture Notes POLAR COORDINATES
PHYS 419: Classical Mechanics Lecture Notes POLAR COORDINATES A vector in two dimensions can be written in Cartesian coordinates as r = xx^ + yy^ (1) where x^ and y^ are unit vectors in the direction of Cartesian axes and x and y are the components of the vector, see also the ¯gure. It is often convenient to use coordinate systems other than the Cartesian system, in particular we will often use polar coordinates. These coordinates are speci¯ed by r = jrj and the angle Á between r and x^, see the ¯gure. The relations between the polar and Cartesian coordinates are very simple: x = r cos Á y = r sin Á and p y r = x2 + y2 Á = arctan : x The unit vectors of polar coordinate system are denoted by r^ and Á^. The former one is de¯ned accordingly as r r^ = (2) r Since r = r cos Á x^ + r sin Á y^; r^ = cos Á x^ + sin Á y^: The simplest way to de¯ne Á^ is to require it to be orthogonal to r^, i.e., to have r^ ¢ Á^ = 0. This gives the condition cos ÁÁx + sin ÁÁy = 0: 1 The simplest solution is Áx = ¡ sin Á and Áy = cos Á or a solution with signs reversed. This gives Á^ = ¡ sin Á x^ + cos Á y^: This vector has unit length Á^ ¢ Á^ = sin2 Á + cos2 Á = 1: The unit vectors are marked on the ¯gure. With our choice of sign, Á^ points in the direc- tion of increasing angle Á. Notice that r^ and Á^ are drawn from the position of the point considered. -
Section 6.7 Polar Coordinates 113
Section 6.7 Polar Coordinates 113 Course Number Section 6.7 Polar Coordinates Instructor Objective: In this lesson you learned how to plot points in the polar coordinate system and write equations in polar form. Date I. Introduction (Pages 476-477) What you should learn How to plot points in the To form the polar coordinate system in the plane, fix a point O, polar coordinate system called the pole or origin , and construct from O an initial ray called the polar axis . Then each point P in the plane can be assigned polar coordinates as follows: 1) r = directed distance from O to P 2) q = directed angle, counterclockwise from polar axis to the segment from O to P In the polar coordinate system, points do not have a unique representation. For instance, the point (r, q) can be represented as (r, q ± 2np) or (- r, q ± (2n + 1)p) , where n is any integer. Moreover, the pole is represented by (0, q), where q is any angle . Example 1: Plot the point (r, q) = (- 2, 11p/4) on the polar py/2 coordinate system. p x0 3p/2 Example 2: Find another polar representation of the point (4, p/6). Answers will vary. One such point is (- 4, 7p/6). Larson/Hostetler Trigonometry, Sixth Edition Student Success Organizer IAE Copyright © Houghton Mifflin Company. All rights reserved. 114 Chapter 6 Topics in Analytic Geometry II. Coordinate Conversion (Pages 477-478) What you should learn How to convert points The polar coordinates (r, q) are related to the rectangular from rectangular to polar coordinates (x, y) as follows . -
A Dynamic Rod Model to Simulate Mechanics of Cables and Dna
A DYNAMIC ROD MODEL TO SIMULATE MECHANICS OF CABLES AND DNA by Sachin Goyal A dissertation submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy (Mechanical Engineering and Scientific Computing) in The University of Michigan 2006 Doctoral Committee: Professor Noel Perkins, Chair Associate Professor Edgar Meyhofer, Co-Chair Assistant Professor Ioan Andricioaei Assistant Professor Krishnakumar Garikipati Assistant Professor Jens-Christian Meiners Dedication To my parents ii Acknowledgements I am extremely grateful to my advisor Prof. Noel Perkins for his highly conducive and motivating research guidance and overall mentoring. I sincerely appreciate many engaging discussions of DNA mechanics and supercoiling with Prof. E. Meyhofer and Prof. K. Garikipati in Mechanical Engineering Program, Prof. C. Meiners in the Biophysics Program, Prof. I. Andricioaei in the Biochemistry/ Biophysics Program and and Dr. S. Blumberg in Medical school at the University of Michigan and Dr. C. L. Lee at the Lawrence Livermore National Laboratory, California. I also appreciate Professor Jason D. Kahn (Department of Chemistry and Biochemistry, University of Maryland) for providing the sequences used in his experiments, and Professor Wilma K. Olson (Department of Chemistry and Chemical Biology, Rutgers University) for suggesting alternative binding topologies in DNA-protein complexes. I also acknowledge recent graduate students T. Lillian in Mechanical Engineering Program, D. Wilson in Physics Program and J. Wereszczynski in Chemistry Program to extend my work and collaborate on ongoing studies beyond the scope of dissertation. I also gratefully acknowledge the research support provided by the U. S. Office of Naval Research, Lawrence Livermore National Laboratories, and the National Science Foundation. -
A Survey of the Development of Geometry up to 1870
A Survey of the Development of Geometry up to 1870∗ Eldar Straume Department of mathematical sciences Norwegian University of Science and Technology (NTNU) N-9471 Trondheim, Norway September 4, 2014 Abstract This is an expository treatise on the development of the classical ge- ometries, starting from the origins of Euclidean geometry a few centuries BC up to around 1870. At this time classical differential geometry came to an end, and the Riemannian geometric approach started to be developed. Moreover, the discovery of non-Euclidean geometry, about 40 years earlier, had just been demonstrated to be a ”true” geometry on the same footing as Euclidean geometry. These were radically new ideas, but henceforth the importance of the topic became gradually realized. As a consequence, the conventional attitude to the basic geometric questions, including the possible geometric structure of the physical space, was challenged, and foundational problems became an important issue during the following decades. Such a basic understanding of the status of geometry around 1870 enables one to study the geometric works of Sophus Lie and Felix Klein at the beginning of their career in the appropriate historical perspective. arXiv:1409.1140v1 [math.HO] 3 Sep 2014 Contents 1 Euclideangeometry,thesourceofallgeometries 3 1.1 Earlygeometryandtheroleoftherealnumbers . 4 1.1.1 Geometric algebra, constructivism, and the real numbers 7 1.1.2 Thedownfalloftheancientgeometry . 8 ∗This monograph was written up in 2008-2009, as a preparation to the further study of the early geometrical works of Sophus Lie and Felix Klein at the beginning of their career around 1870. The author apologizes for possible historiographic shortcomings, errors, and perhaps lack of updated information on certain topics from the history of mathematics. -
1.7 Cylindrical and Spherical Coordinates
56 CHAPTER 1. VECTORS AND THE GEOMETRY OF SPACE 1.7 Cylindrical and Spherical Coordinates 1.7.1 Review: Polar Coordinates The polar coordinate system is a two-dimensional coordinate system in which the position of each point on the plane is determined by an angle and a distance. The distance is usually denoted r and the angle is usually denoted . Thus, in this coordinate system, the position of a point will be given by the ordered pair (r, ). These are called the polar coordinates These two quantities r and , are determined as follows. First, we need some reference points. You may recall that in the Cartesian coordinate system, everything was measured with respect to the coordinate axes. In the polar coordinate system, everything is measured with respect a fixed point called the pole and an axis called the polar axis. The is the equivalent of the origin in the Cartesian coordinate system. The polar axis corresponds to the positive x-axis. Given a point P in the plane, we draw a line from the pole to P . The distance from the pole to P is r, the angle, measured counterclockwise, by which the polar axis has to be rotated in order to go through P is . The polar coordinates of P are then (r, ). Figure 1.7.1 shows two points and their representation in the polar coordinate system. Remark 79 Let us make several remarks. 1. Recall that a positive value of means that we are moving counterclock- wise. But can also be negative. A negative value of means that the polar axis is rotated clockwise to intersect with P .